High energy nuclear interactions are usually treated in
the Glauber theory [1]}, [2]}, [3]}.
It is highly efficient in describing
the hadron-nucleus scattering where all the relevant diagrams
can be summed up in the closed form. The nucleus-nucleus scattering
becomes rapidly more complicated for \(A>4\)  and additional simplified
approximations are usually made to get the result analytically.
An example of such calculations for the differential elastic
and reaction cross sections for \(^{11}\) Li – \(^{12}\) C scattering
can be found in Refs. [4]}, [5]}.
